c
Statement-\(I\)

\(\mathrm{I}_{\mathrm{m}}=\frac{\mathrm{V}_{\mathrm{m}}}{\sqrt{\mathrm{R}^2+\left(\mathrm{X}_{\mathrm{L}}-\mathrm{X}_{\mathrm{C}}\right)^2}}\) at resonance \(\mathrm{X}_{\mathrm{L}}=\mathrm{X}_{\mathrm{C}}\)

Thus, \(I_m=\frac{V_m}{R}\)

\(\because\) Impendence is minimum therefore \(I\) is maximum at resonance.

Statement-\(II\)

\(\mathrm{I}=\left(\frac{\mathrm{V}}{\mathrm{R}}\right)\) in purely resistive circuit.